Download Report

R. Tugrul Ogulata,
Serin Mavruz
The University of Cukurova,
Department of Textile Engineering,
01330 Adana, Turkey
E-mail: ogulata@cu.edu.tr
smavruz@cu.edu.tr
Investigation of Porosity and Air
Permeability Values of Plain Knitted Fabrics
Abstract
The air permeability of a fabric is defined as the amount of air passed over a surface under a
certain pressure difference in a unit time. This value has significance with respect to the usage
area. Since knitted fabrics have a loop structure, they have more pores than woven fabrics;
therefore, in general, the air permeability of knitted fabrics is higher than that of woven fabrics
of the same weight. An experiment to determine the air permeability is very important as it
defines the properties of keeping warm, protection against the wind, breathability etc. of knitted fabrics used as clothing. In this study, it has been attempted to establish a theoretical model
for the porosity and predicted air permeability of plain knitted fabrics. A theoretical model was
created to predict the porosity and air permeability of a knitted structure depending on the geometrical parameters, such as the courses per cm, wales per cm, stitch length, fabric thickness,
yarn count, diameter of yarn and fiber density. For this purpose, a theoretical model of porous
systems based on D’Arcy’s law was used, the validity of which was confirmed by experimental
results using 100% cotton plain knitted fabrics produced from ring and compact yarns of different yarn number linear density and tightness.
Key words: knitted structure, porosity, air permeability, geometric modelling.
Designations used
A1
At
c
dh
dp
dy
f
m
n
Q
R
Re
rp
ry
t
Um
w
r
ry
e
v
h
DP
l
- cross-sectional area of pore, cm2
- fabric area tested, cm2
- number of courses per centimeter
- hydraulic diameter of a pore, cm
- pore diameter, cm
- yarn diameter, cm
- friction coefficient
- number of pores per square
- coefficient indicating the flow regime
- total flow rate of the air, m3/s
- air permeability, mm/s
- Reynolds number
- pore radius, cm
- yarn radius, cm
- fabric thickness, cm
- mean air flow velocity, m/s
- number of wales per centimeter
- air density, kg/m3
- yarn density, g/cc
- rate of void area
- kinematic viscosity of the air, m2/s
- dynamic viscosity of the air, Pa.s
- pressure drop, Pa
- coefficient of laminar and turbulent
flow
n Introduction
Knitting is the process of forming fabric
by interloping yarn in a series of connected loops using needles. Knit fabrics provide outstanding comfort qualities and
have long been preferred in many types
of clothing. In addition to comfort imparted by the extensible looped structure,
knits also provide lightweight warmth,
wrinkle resistance, and ease of care [1].
Such knitted structures have a more open
character when compared to other textile fabric structures, such as woven and
braided [2].
Air permeability is often used in evaluating and comparing the ‘breathability’
of various fabrics (coated and uncoated)
for such end uses as raincoats, tents and
uniform shirtings. It helps evaluate the
performance of parachutes sails, vacuum
cleaners, air bags, sail cloth and industrial filter fabrics [3 - 6].
counts per unit area are the main factors
affecting the porosity of textiles. The porosity of a fabric is connected with certain of its important features, such as air
permeability, water permeability, dyeing
properties etc. [9, 10].
Air permeability is defined as the volume
of air in liters which is passed through
100 cm2 (10 cm × 10 cm) of the fabric
in one minute at a pressure difference of
10 mm head of water [7].
Most of the previous studies investigated
the relationship between the air permeability and structural characteristics of
plain knitted fabrics. For example, Oinuma (1990) showed that the stitch length,
porosity and air permeability increase
and the thermal retaining property decreases for dry relaxed cotton 1 × 1 rib
knitted fabrics [11]. Marmarali (2003)
investigated the air permeability of cotton/spandex single jersey fabrics within
their dimensional and physical properties
and compared results with fabrics knitted
from cotton alone. It proved that the air
permeability of fabrics containing spandex was lower [12]. Karaguzel (2004)
calculated values of pore size and pore
volume for plain knitted fabrics. Those
of the pore size were measured with image analysis and fluid extrusion procedures. It was found that there was a noticeable difference between the estimated
and measured values [8]. On the basis of
computer image analysis, the surface porosity of knitted fabrics was evaluated for
plain double-layered and lining knitted
fabrics by Wilbik-Halgas et al. (2006). It
was found that air permeability, contrary
to water vapour permeability, is a function of the thickness and surface porosity
of knitted fabrics [13]. Benltoufa et al.
(2007) investigated methods of determining jersey porosity, which proved that
geometry modelling is the most suitable
and easiest method of determining poros-
Due to the manner in which yarns and
fabrics are constructed, a large proportion of the total volume occupied by a
fabric is usually airspace. The distribution of this airspace influences a number
of important fabric properties such as
warmth and protection against wind and
rain in clothing, and the efficiency of filtration in industrial cloths.
Air permeability is an important factor in
the comfort of a fabric as it plays a role
in transporting moisture vapour from the
skin to the outside atmosphere. The assumption is that vapour travels mainly
through fabric spaces by diffusion in air
from one side of the fabric to the other [8].
The porosity of a knitted structure will influence its physical properties, such as the
bulk density, moisture absorbency, mass
transfer and thermal conductivity [2].
Air flow through textiles is mainly affected by the pore characteristics of fabrics.
It is quite clear that pore dimension and
distribution is a function of fabric geometry. The yarn diameter, surface formation techniques and the number of loop
Ogulata R. T., Mavruz S.; Investigation of Porosity and Air Permeability Values of Plain Knitted Fabrics.
FIBRES & TEXTILES in Eastern Europe 2010, Vol. 18, No. 5 (82) pp. 71-75.
71
W
A
B
C
Course
Wale
Wales/cm
= 1/W=w
Courses/cm = 1/C=c
Stitch length = AB= l
Stitches/cm 2 = S (c×w)
Figure 1. Representation of a plain knitted
fabric.
were taken into account in the calculation of air permeability. Three factors are
mainly considered that are related to the
pores in fabrics.
1) Cross-sectional area of each pore,
2) Depth of each pore or the thickness of
the fabric and
3) The number of pores per unit area or
the number of courses and wales per
unit area.
In this work, these parameters are considered to develop a theoretical model for
porosity and air permeability.
Figure 2. Stitch diagram of a plain knitted
structure.
ity [14]. The thermal properties and thermal behaviour of cellulose textile fabrics
(air permeability, porosity) were investigated by Stankovic et al. (2008), in which
they found that air permeability and heat
transfer through fabrics is closely related
to both the capillary structure and surface
characteristics of yarns [15].
Dias and Delkumburewatte, (2008) created a theoretical model to predict the porosity of a knitted structure. It was determined that porosity depended on fabric
parameters and relaxation progression [2].
Mavruz and Ogulata, (2009) investigated air permeability of cotton knitted fabrics.
Before manufacturing the fabrics the
equation of regression was used to predict air permeability, depending on some
fabric properties [16].
Establishing a more complex theory to
express air permeability related to all
fabric parameters will have difficulties.
To simplify the matter, certain important
parameters such as the pore of the fabric
72
A knitted fabric consists of one or more
looped yarns. Plain knitted fabric, which
is illustrated in Figure 1, is one structure of knitted fabric. In this paper, we
consider plain knitted fabrics which are
commonly used in many apparel applications. W and C represent wale and
course spacing, whereas w and c correspond to the number of wales per cm and
number of courses per cm, respectively
[17]. (Wales per cm: the number of visible loops per unit length in cm measured along a course. Courses per cm: the
number of visible loops per unit length in
cm measured along a wale. Stitch length:
the length of yarn in a knitted loop).
When considering fluid flow through
textiles, the shape arrangement and size
distribution of voids through which the
fluid flows are of great importance. The
fabric thickness and differential pressure
between the two surfaces of a fabric are
the other dominant factors that affect permeability. The pressure gradient through
a textile is a function of the viscosity,
density, rate of fluid flow and porosity, as
in the case of flow through a pipe [9].
The dependence of the friction coefficient, f, on the Reynolds Number, Re, for
laminar and turbulent flow is described
by the Blasius equation:
f = l . Re-n
U m .d h
(2)
where Um is the mean flow velocity, dh
the hydraulic diameter of a pore, and v is
the kinematic viscosity of the air [4, 18].
R
e =
Re
(1)
where λ is the coefficient of laminar or
turbulent flow, and n is a coefficient indicating the flow regime.
Laminar flow:
λ = 64, n = 1
Turbulent flow: λ = 0.3164, n = 0.25
The type of flow depends on the Reynolds number. The Reynolds number
represents the ratio of the inertia force to
the viscous force [4].
ν
The pressure drop of the flow through
a duct over the thickness of the fabric
is related to the friction factor f through
D’Arcy’s formulation.
DP = f
n Theoretical Model
Pore of a unit cell
The Reynolds number is calculated as
follows:
t U m2
(3)
r
dh
2
where t is the thickness of the fabric, and r is the air density [19].
Knitted fabric has a porous structure. For
this reason, the air velocity in pores must
be taken into consideration.
U=
Um
e
(4)
where U is the air velocity through pores,
and e is rate of the void area (porosity) [4].
Figure 2 shows the pore within a loop.
Our theoretical model was created by
considering one repeating unit cell of
a knitted structure. By determining the
course (c) per cm, wale (w) per cm,
thickness (t), yarn diameter (dy) and loop
length (l), the porosity can be shown as
follows [14]:
e = 1−
Yarnvolume
(5)
Totalvolume
2
2
Yarn volume = pd y 2l = pd y l (6)
4
Total volume =
2
11
t
(7)
t=
c w cw
cw
Finally,
e = 1−
pd y2 lcw (8)
2t
The air velocity through pores of the fabric does not usually have a high value.
Therefore, the fluid flow in the pores is
laminar. According to kinetic theory, if
the Reynolds number is below 2320, the
flow in the tube is laminar [4, 18]. For
this reason, the mean air velocity through
one pore can be expressed as:
 d2 
U m =  h DP (9)
32 ht 
 32
The flow rate of air for a fabric of porous
material, Q, becomes:
FIBRES & TEXTILES in Eastern Europe 2010, Vol. 18, No. 5 (82)
Q = m . A1 . U (10)
where m is the number of pores, and A1
is the cross-sectional area of the pore [4]
A1 = p
d
2
p
4
(11)
where, dp is the pore diameter (In this
study, the loops are assumed to be composed of ideal yarns which are circular in
cross-section and have a constant diameter throughout their length. Yarn deformation at the crossover points is omitted,
hence it is accepted that dp = dh).
Thus, equation (10) can be written as follows:
4
Q = m p d p 1010−6 DP (m3/s) (12)
e 128ht
The value of air permeability (R) is calculated according to the following equation
R=
Q
(13)
At
where At is the fabric area tested [7].
n Materials and methods
In order to compare the values of air
permeability from theoretical modelling and those from experiments of air
permeability, we produced 18 (eighteen)
knitted samples with various knitting parameters. The yarns were made of cotton
fibers, and the bonding type of each sample was plain. Plain knitted fabrics were
knitted with three different tightnesses
(slack, medium and tight) on a circular
knitting machine using ring and compact
yarns of 19.72, 14.79 and 11.83 tex.
(14)
Figure 3. Representation of yarn in 1 cm2
of fabric; ry - yarn radius, rp - pore radius,
ry - yarn density (Pierce used a value of
0.909 g/cc for cotton yarn), T - yarn linear
density in tex.
19.72 tex
types, we repeated this measurement for
ten (10) samples, thus obtaining a body
of (18 × 10 =) 180 measurements. Furthermore, the loop length, wales per cm,
courses per cm, thickness and weight of
the fabrics were measured according to
the relevant standards [20 - 23].
14.79 tex
11.83 tex
Ring
T
ppp
r yy 10
10 55
l×S
l×S
The knitted samples were conditioned
for 48 hours in atmospheric conditions
of 20 ± 2 °C temperature and 65 ± 2%
relative humidity before the tests were
performed. The air permeability of the
samples in mm/s was measured according to the method specified by Standard TS 391 EN ISO 9237 [8], using a
Textest FX 3300 air permeability tester.
The measurements were performed at a
constant pressure drop of 100 Pa (20 cm2
test area). For each one of the 18 fabric
dp is calculated from Figure 3 (yarn representation) and Figure 1.
ry =
ry
1
Volume of free space (cm3) in
of fabric = 1×1×t = t - Slpry2 (16)
cm2
Area of free space (cm2) in
t - Slpr 22 (17)
1 cm2 of fabric = − Sl pryy t
Area of open space within
- Slpr 22 (18)
one loop = t − Sl pryy tStS
As mentioned beforehand, if the area occupied by a pore is transformed to that of
a circle, the pore radius (rp) can be written as equation 19 [8].
22
yy
pr (19)
rp = tt−- SlSlpr
pptS
tS
As indicated by equation 19, when the
stitch density, stitch length or yarn diameter increases, pore size values decrease.
The equations developed in this study
will be used to predict the pore size and
air permeability of plain knitted fabrics.
FIBRES & TEXTILES in Eastern Europe 2010, Vol. 18, No. 5 (82)
Compact
Volume of yarn in 1 cm2 = Slpry2 (15)
Figure 4. Microscopic views of the yarns.
Table 1. Fabric properties and experimental air permeability values.
Sample
number
Yarn type
Yarn
R: Ring
number,
C: Compact
tex
Loop
length,
cm
Course
count
per cm
Wale
count
per cm
Thickness,
cm
Weight,
g/m2
Experimental
air permeability, mm/s
1
R
19.72
0.255
23.0
12.3
0.0069
161.38
1193
2
R
19.72
0.285
18.0
12.3
0.0057
136.78
1562
3
R
19.72
0.320
16.0
12.1
0.0068
136.90
1562
4
C
19.72
0.260
24.0
13.0
0.0060
159.48
1532
5
C
19.72
0.286
19.0
13.0
0.0058
143.72
1647
6
C
19.72
0.330
15.0
13.0
0.0062
134.22
1948
7
R
14.79
0.256
24.0
12.2
0.0063
120.88
2020
8
R
14.79
0.284
19.0
12.0
0.0059
105.72
2077
9
R
14.79
0.320
15.0
12.0
0.0052
87.22
3059
10
C
14.79
0.261
24.0
13.0
0.0059
126.10
2459
11
C
14.79
0.280
18.0
13.0
0.0060
118.24
2966
12
C
14.79
0.250
15.0
13.0
0.0065
107.16
3708
13
R
11.83
0.250
23.0
13.0
0.0053
86.98
2938
14
R
11.83
0.280
18.0
14.0
0.0053
75.86
3502
15
R
11.83
0.320
16.0
12.0
0.0061
76.62
3680
16
C
11.83
0.251
24.0
13.0
0.0052
98.30
3128
17
C
11.83
0.290
18.0
13.0
0.0056
89.58
3306
18
C
11.83
0.330
15.0
12.0
0.0060
76.82
4616
73
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
Figure 5. Microscopic views of the knitted structure.
Fabric properties (yarn number, loop
length, course count per cm, wale count
per cm, thickness, weight) and the (experimental) air permeability values
measured are presented in Table 1.
It can be seen that the fabrics differed in
terms of the yarn linear densities, yarn
type, courses per cm and loop length.
The thickness of the fabrics varied with
the loop length and course count. Since
the wale count per cm usually depends
on the machine settings, a constant range
from 12 - 13 should be maintained.
According to Table 1, the fabric with
the lowest course count per cm and yarn
number in tex has the highest air permeability values. Therefore, the rising loop
length resulted in a looser surface on the
fabric, thereby increasing the air permeability.
In order to predict air permeability values
for the knitted fabrics, the following were
used: values of the porosity, the radius of
pores and yarns, and the flow rate calculated using the newly developed equations expressed in the theoretical model.
Moreover, we observed microscopic
views of the yarns and pores in the knitted fabrics from pictures taken using an
image analysis device (Figure 4 and 5).
Sample numbers were marked on the pictures in Figure 5.
In Figure 4 it can be seen that as the yarn
count decreased, yarn hairiness values
fell in general. Furthermore, microscopic
views revealed that the surface of knitted
samples produced from thin yarns (both
74
ring and compact yarns) is highly nonuniform with deformations (especially
in loose fabrics) because of the bigger
pore dimensions (Figure 5). As is widely
known, the compact spinning method
forms a different yarn structure. The most
evident properties of these yarns are their
high breaking strength, high elongation
and low hairiness. Moreover, other yarn
properties such as yarn unevenness, thin/
thick places etc. are comparable to those
of conventional ring yarn. As the surface
of compact yarns is smoother and less
hairy, fabrics produced from such yarns
cannot block air, thus indicating high air
permeability. However, the difference
between compact and conventional ring
yarns is not too great.
In order to simplify the theoretical calculations, loops are assumed to be composed of ideal yarns but with great variability in pore size distribution. Thus samples produced with 14.79 and 11.83 tex
yarns have pore dimensions which are
highly variable across the fabric. It is
difficult to estimate the porosity of fabrics by calculating the pore dimensions
Air permeability, mm/s
n Results and discussion
5000
4500
4000
3500
3000
2500
2000
1500
1000
500
0
experimental
1
2
3
4
5
and yarn diameter. As is known, yarns in
the structure of the fabric do not have a
smooth surface nor a solid construction.
There is also a lot of emptiness in the
yarns. Consequently, in order to obtain
closer results, the value of the pore diameter of knitted fabrics produced from
14.79 and 11.83 tex yarns was increased
by 15%, and these new values were used
for calculations.
Comparing the theoretical model method
(Equation 13) and that using experimental air permeability values, we obtained the result shown in Figure 6 (see
page 109).
The match is close, which is also indicated by the high values of correlation
coefficient, R2, obtained from the statistical analysis. Figure 7 shows correlation
plots between the predicted and measured values (x axis-measured values, y
axis-predicted values).
The values in Figure 7 indicate that the
correlation for fabrics produced from
19.72 tex yarn is superior to that for fab-
theoretical
6
7
8
9
10
11
12
13
14
15
16
17
18
Sample no
Figure 6. Air permeability values according to the experimental and theoretical models.
FIBRES & TEXTILES in Eastern Europe 2010, Vol. 18, No. 5 (82)
4000
4000
2
R = 0.81
2
predicted values
predicted
R = 0.87
3000
2000
1000
1000
2000
3000
4000
5000
3000
2000
1000
0.03
Figure 7. Correlation plots for predicted and measured values.
Moreover, as demonstrated in Figure 8,
there is a near positive linear relationship between pore size and predicted air
permeability values. Thus, the higher the
pore sizes, the higher the air permeability.
n Conclusion
An experimental study was carried out to
develop a theoretical model to predict air
permeability values for knitted fabrics.
The theoretical model predicts the value
of the air permeability using the pore size
and some fabric properties before manufacturing.
D’Arcy’s formulation was used to establish an equation expressing the relationship between the air permeability of
knitted fabrics and fabric structure parameters.
According to the experimental results,
the fabric with the lowest course count
per cm and yarn number in tex has the
highest air permeability values. Moreover, increasing the loop length produced a
looser surface in the fabric and increased
air permeability. As the yarn gets thinner
and the pores between loops get larger,
the air permeability will increase accordingly. According to some formulations,
when the stitch density, stitch length or
yarn diameter increase, pore size values
decreases.
Due to the differences between ideal and
real geometry and the random variation
of the fabric structure, there are no exact
dependences between experimental air
permeability and predicted air permeabilFIBRES & TEXTILES in Eastern Europe 2010, Vol. 18, No. 5 (82)
0.05
0.06
0.07
0.08
0.09 0.10
pore size
measured
rics produced from 14.83 and 11.92 tex
yarns. Air permeability in knitted fabrics
is related to pore size. As discussed earlier, variability in pore size affects permeability values.
0.04
Figure 8. Relationship between predicted air permeability values
and pore size.
ity values. However, the closeness of the
results of predictions based on calculated
values from the theoretical model and
experimental values show that our model
can be successfully used for the prediction of the air permeability of knitted
fabrics (R2 = 0.87). This model is simple
and efficient.
Permeability and porosity are strongly
related to each other. If a fabric has very
high porosity, it can be assumed that it is
permeable. It was also found that there
is a near positive linear relationship between pore size and air permeability
values (R2 = 0.81), hence tt could be assumed that the model developed is applicable for predicting the air permeability
of plain knitted fabrics produced with
different fiber types.
References
1.Tou N. A.; An Investigation of Arcing in
Two Structure Weft Knit Fabrics, MSc
Thesis, North Carolina State University,
Textile & Apparel Technology & Management, 2005.
2.Dias T., Delkumburewatte G. B.; Fibers
and Polymers, Vol. 9, No. 1 (2008) pp.
76-79.
3.Air Permeability Test Method & Explanatory Notes, www.awta.com.au, 2008.
4.Ogulata R. T.; Journal of Textile and Apparel, Technology and Management, Volume 5, Issue 2 (2006) pp. 1-10.
5.Tokarska M.; Fibres & Textiles in Eastern
Europe, Vol. 16, No. 1 (66), 2008 pp. 76-80.
6.Ogulata R. T, Koc E.; Association for the
Advancement of Modelling & Simulation
Techniques in Enterprises, Vol. 70, No.
8, (2001) pp. 39-48.
7.TS 391 EN ISO 9237, Textiles-Determination of the Permeability of Fabrics to
Air, Turkish Standards Institution, Ankara,
1999.
8.K araguzel B.; Characterization and
Role of Porosity in Knitted Fabrics, MSc
Thesis, North Carolina State University,
Department of Textile Engineering, Chemistry and Science, 2004.
9.Cay A., Vassiliadis S., Rangoussi M.,
Tarakcioglu I.; International Journal of
Signal Processing, Vol. 1, Number 1,
2004 pp. 51-54.
10.Cay A., Tarakcioglu I.; Journal of the
Textile Institute, Vol. 99, Issue 6, (2008)
pp. 499-504.
11.Oinuma R., Journal of the Textile Machinery Society of Japan, Vol. 36, No. 3,
1990, pp. 91-95.
12.Marmarali A. B.; Textile Research Journal, 73(1) 2003, pp. 11-14.
13.Wilbik-Halgas B., Danych R., Wiecek B.,
Kowalski K.; Fibres & Textiles in Eastern
Europe, Vol. 14, No. 3(57) 2006, pp. 77-80.
14.Benltoufa S., Fayala F., Cheikhrouhou
M., Ben Nasrallah, S., AUTEX Research
Journal, Vol. 7, No. 1, 2007 pp. 63-69.
15.Stankovic S. B., Popovic D., Poparic G.
B.; Polymer Testing, Vol. 27, No. 1, 2008
pp. 41-48.
16.Mavruz S., Ogulata R. T.; Tekstil ve Konfeksiyon, Vol. 19, No. 1. 2009, pp. 29-38.
17.Booth J. E., Textile Mathematics, The
Textile Institute, ISBN 0 900739 24X, p.
514, 1977.
18.Xu G., Wang F.; Journal of Industrial Textiles, Vol. 34, No: 4, 2005 pp. 243-254.
19.Holman J. P.; Heat Transfer, Seventh
Edition, McGraw-Hill Book Company,
1992.
20. TS EN 14970, Textiles - Knitted fabrics Determination of Stitch Length and Yarn
Linear Density in Weft Knitted Fabrics,
Turkish Standards Institution, Ankara,
2006.
21. TS EN 14971, Textiles - Knitted fabrics
- Determination of Number of Stitches
per Unit Length and Unit Area, Turkish
Standards Institution, Ankara, 2006.
22. TS 7128 EN ISO 5084, Textiles-Determination of Thickness of Textiles and Textile
Products, Turkish Standards Institution,
Ankara, 1998.
23. TS 251, Determination of Mass per Unit
Length and Mass per Unit Area, Turkish
Standards Institution, Ankara, 1991.
Received 29.12.2008
Reviewed 17.09.2009
75